TY - JOUR
T1 - High thermoelectricpower factor in graphene/hBN devices
AU - Duan, Junxi
AU - Wang, Xiaoming
AU - Lai, Xinyuan
AU - Li, Guohong
AU - Watanabe, Kenji
AU - Taniguchi, Takashi
AU - Zebarjadi, Mona
AU - Andrei, Eva Y.
PY - 2016/12/13
Y1 - 2016/12/13
N2 - Fast and controllable cooling at nanoscales requires a combination of highly efficient passive cooling and active cooling. Although passive cooling in graphene-based devices is quite effective due to graphene's extraordinary heat conduction, active cooling has not been considered feasible due to graphene's low thermoelectric power factor. Here, we show that the thermoelectric performance of graphene can be significantly improved by using hexagonal boron nitride (hBN) substrates instead of SiO2. We find the room temperature efficiency of active cooling in the device, as gauged by the power factor times temperature, reaches values as high as 10.35 W·m-1·K-1, corresponding to more than doubling the highest reported room temperature bulk power factors, 5 W·m-1·K-1, in YbAl3, and quadrupling the best 2D power factor, 2.5W·m-1·K-1, in MoS2. We further show that the Seebeck coefficient provides a direct measure of substrate-induced random potential fluctuations and that their significant reduction for hBN substrates enables fast gate-controlled switching of the Seebeck coefficient polarity for applications in integrated active cooling devices.
AB - Fast and controllable cooling at nanoscales requires a combination of highly efficient passive cooling and active cooling. Although passive cooling in graphene-based devices is quite effective due to graphene's extraordinary heat conduction, active cooling has not been considered feasible due to graphene's low thermoelectric power factor. Here, we show that the thermoelectric performance of graphene can be significantly improved by using hexagonal boron nitride (hBN) substrates instead of SiO2. We find the room temperature efficiency of active cooling in the device, as gauged by the power factor times temperature, reaches values as high as 10.35 W·m-1·K-1, corresponding to more than doubling the highest reported room temperature bulk power factors, 5 W·m-1·K-1, in YbAl3, and quadrupling the best 2D power factor, 2.5W·m-1·K-1, in MoS2. We further show that the Seebeck coefficient provides a direct measure of substrate-induced random potential fluctuations and that their significant reduction for hBN substrates enables fast gate-controlled switching of the Seebeck coefficient polarity for applications in integrated active cooling devices.
KW - Electron-hole puddles
KW - Graphene
KW - Screened coulomb scattering
KW - Seebeck coefficient
KW - Thermoelectric power factor
UR - http://www.scopus.com/inward/record.url?scp=85006026408&partnerID=8YFLogxK
U2 - 10.1073/pnas.1615913113
DO - 10.1073/pnas.1615913113
M3 - Article
AN - SCOPUS:85006026408
SN - 0027-8424
VL - 113
SP - 14272
EP - 14276
JO - Proceedings of the National Academy of Sciences of the United States of America
JF - Proceedings of the National Academy of Sciences of the United States of America
IS - 50
ER -